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    Dual Carbamoylations on the Polyketide and Glycosyl Moiety by Asm21 Result in Extended Ansamitocin Biosynthesis

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    SummaryCarbamoylation is one of the post-PKS modifications in ansamitocin biosynthesis. A novel ansamitocinoside with carbamoyl substitution at the C-4 hydroxyl group of the N-Ξ²-D-glucosyl moiety was identified from the ansamitocin producer, Actinosynnema pretiosum. Through biotransformation, the carbamoyltransferase gene asm21 was suggested to be responsible for the carbamoylation of the glucosyl moiety. Three new derivatives without the backbone carbamoyl group were isolated from an asm21 mutant and characterized by NMR spectroscopy. Among them, 18-O-methyl-19-chloroproansamitocin was the major product and the preferred substrate for macrolactam C-7 carbamoylation by Asm21. However, Asm21 exhibited higher catalytic efficiency toward the glucosyl moiety. Furthermore, the dual carbamoylations and N-glycosylation were precisely demonstrated inΒ vivo. This work represents the first biochemical characterization of an O-carbamoyltransferase performing dual actions on both a polyketide backbone and a glycosyl moiety during ansamitocin biosynthesis

    Testing the light scalar meson as a non-qqˉq\bar q state in semileptonic DD decays

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    To distinguish between the normal qqΛ‰q\bar q and exotic diquark-antidiqark (q2qΛ‰2q^2\bar q^2) contents of the lowest-lying scalar meson (S0S_0), we investigate the semileptonic Dβ†’S0e+Ξ½e,S0β†’M1M2D\to S_0 e^+\nu_e, S_0\to M_1 M_2 decays, where M1(2)M_{1(2)} represents a pseudoscalar meson. With the form factors extracted from the current data, we calculate B(Ds+β†’Οƒ0e+Ξ½e,Οƒ0β†’Ο€0Ο€0)=(12.9βˆ’4.9+6.3)Γ—10βˆ’4{\cal B}(D_s^+\to \sigma_0 e^+\nu_e,\sigma_0\to\pi^0\pi^0) =(12.9^{+6.3}_{-4.9})\times 10^{-4} and (0.8βˆ’0.7+1.2)Γ—10βˆ’4(0.8^{+1.2}_{-0.7})\times 10^{-4} for the qqΛ‰q\bar q and q2qΛ‰2q^2\bar q^2 quark structures, respectively, and compare them to the experimental upper limit: 6.4Γ—10βˆ’46.4\times 10^{-4}. It is clearly seen that S0S_0 prefers to be the q2qΛ‰2q^2\bar q^2 bound state. Particularly, BqqΛ‰(Ds+β†’Οƒ0e+Ξ½e,Οƒ0β†’Ο€+Ο€βˆ’)=(25.8βˆ’β€…β€Šβ€‰9.8+12.5)Γ—10βˆ’4{\cal B}_{q\bar q}(D_s^+\to \sigma_0 e^+\nu_e,\sigma_0\to\pi^+\pi^-) =(25.8^{+12.5}_{-\;\,9.8})\times 10^{-4} and Bq2qΛ‰2(Ds+β†’Οƒ0e+Ξ½e,Οƒ0β†’Ο€+Ο€βˆ’)=(1.5βˆ’1.3+2.4)Γ—10βˆ’4{\cal B}_{q^2\bar q^2}(D_s^+\to \sigma_0 e^+\nu_e,\sigma_0\to\pi^+\pi^-) =(1.5^{+2.4}_{-1.3})\times 10^{-4} are predicted to deviate far from each other, useful for a clear experimental investigation.Comment: 10 pages, 1 figure, 1 tabl
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